Ismail Ocsoy*abc,
Nuran Isikland,
Sena Cansiza,
Nalan Özdemire and
Weihong Tan*a
aCenter for Research at the Bio/Nano Interface, Department of Chemistry, Shands Cancer Center, UF Genetics Institute, McKnight Brain Institute, University of Florida, Gainesville, Florida 32611, USA. E-mail: ismailocsoy@erciyes.edu.tr
bDepartment of Analytical Chemistry, Faculty of Pharmacy, Erciyes University, Kayseri, 38039 Turkey
cNanotechnology Research Center (ERNAM), Erciyes University, Kayseri, 38039 Turkey
dDepartment of Chemistry, Science and Arts Faculty, Kırıkkale University, Kırıkkale, 7100 Turkey
eDepartment of Chemistry, Faculty of Science, Erciyes University, Kayseri, 38039 Turkey
First published on 18th March 2016
Aptamer-functionalized magnetic graphene oxide conjugates loaded with indocyanine green (ICG) dye, or Apt@ICG@mGO, have been successfully developed for dual-targeted photothermal and photodynamic therapy. In general, a drug or its carrier or their dosage can be important issues in terms of toxicity. However, in this system, each component used is quite safe, biocompatible and clean. For instance, ICG, a Food and Drug Administration (FDA) approved near-infrared (NIR) dye, serves as both a photothermal and photodynamic agent. It is immobilized on the surface of mGO via a physical interaction called “π–π stacking”. The mGO, as a most biocompatible member of the carbo family, is selected for use as a platform for aptamer and ICG dye conjugation, as well as a photothermal agent. The light in the near-infrared region (NIR) was chosen as a harmless light source for activating the agents for photothermal therapy (PTT) and photodynamic therapy (PDT). The magnetic properties of mGO are also used for separation of Apt@ICG@mGO conjugates from the reaction medium. Aptamer sgc8 acts as a targeting ligand to selectively and specifically bind to a protein on the membrane of cancer cell line CCRF-CEM. After the aptamer-functionalized ICG@mGO conjugates are incubated with target CEM cells at 37 °C for 2 hours, they are bound to cells or they may be internalized into the cell via endocytosis. More significantly, we demonstrated that the Apt@ICG@mGO conjugates produce heat for photothermal therapy (PTT) and singlet oxygen for photodynamic therapy (PDT) upon NIR laser irradiation at 808 nm. Thus, remarkably efficient cancer cell destructions with ∼41% and ∼60% and ∼82% cell killing using 10, 50 and 100 ppm Apt@ICG@mGO, respectively are achieved in 5 min light exposure.
In PTT, certain NPs, such as gold nanorods,15–18 nanoshells,19,20 nanocages,21,22 nano-popcorns,23 carbon nanohorns24 and graphene25,26 have been employed as photothermal agents. They efficiently absorb light in the near-infrared region (NIR) and rapidly convert it into heat. Eventually, this rapid local temperature increase in the microenvironment induced by NIR irradiation results in irreversible cell damage and cell death in the range of 42 and 47 °C.27
PDT, also known as light-activated therapy, is a noninvasive medical model that causes cell destruction in the presence of reactive oxygen species (ROS), such as singlet oxygen, generated by irradiation of a photosensitizer (PS).28–30 In PDT, PS molecules are irradiated with light at an appropriate wavelength, and the excited PS transfers photon energy to surrounding oxygen molecules to generate highly reactive singlet oxygen. The singlet oxygen molecule, as a cytotoxic agent, attacks target cells and induces irreversible damage. Both PTT and PDT have several advantages over conventional chemotherapy because they are noninvasive, selective, and relatively inexpensive, have reproducible properties and avoid the related side effects of other therapies.28,31
Indocyanine green (ICG) is an amphiphilic, tricarbocyanine dye, which has been approved by the United States Food and Drug Administration (FDA) for biomedical applications. Its low toxicity and unique optical properties, including its very strong absorption band (780 nm) and effective emission band (800–820 nm), make ICG ideally suited for optical imaging in cells, tissues and small animals.32,33 In the visible region, cell and tissue auto-fluorescence results in weak signal-to-noise ratios in vitro and in vivo, and is thus a major drawback for the generation of high-resolution optical imaging. In contrast, the use of ICG as a NIR agent is vitally important to optical imaging of human vasculature, tissue and cells, which are relatively transparent to NIR radiation (700–1300 nm), allowing deep light penetration up to several centimeters in biological tissues. Recently, ICG has also been used as a PTT and PDT agent for clinical treatment.28–36 When ICG is irradiated with an appropriate wavelength, it can generate heat for PTT and singlet oxygen for PDT. However, the efficient use of ICG is very limited as a result of the intrinsic disadvantages associated with concentration-dependent aggregation in aqueous solution, such as easy chemical degradation, depending on the nature of the solvent, dye concentration, temperature and light exposure, and the extremely rapid pharmacokinetics of ICG and its nonspecific binding to proteins, including human serum albumin, lipoproteins, plasma proteins and endothelial cells.37,38
Since its discovery in 2004, graphene, which is composed of one or few atom-thick two-dimensional (2D) sp2-bonded carbon sheets, has been extensively used in a broad spectrum of applications owing to its unique physicochemical, mechanical and electronic properties.39 Recently, graphene oxide (GO), the oxidized form of graphene, has been utilized to construct optical, electrical and electrochemical biosensors and to design surface-enhanced Raman scattering (SERS) platforms, in addition to its use as a substrate for matrix-assisted laser desorption/ionization (MALDI), antimicrobial agent40,41 and as a carrier for drug and DNA delivery.42–46 The large surface area of GO, which features many functional groups and domains, as well as its biocompatibility, make GO an ideal platform for efficient conjugation of aromatic biomolecules, such as anticancer drugs, photosensitizers, proteins, peptides and single-stranded DNA, through π–π stacking. Recently, ‘pi-excessive’ or ‘electron-rich’ drugs and photosensitizers have been efficiently loaded on the surface of GO for chemo- and photodynamic therapies.47–49 For instance, Dai and coworker reported on water-insoluble anticancer drugs physically loaded on the GO surface for effective chemotherapy.48 Loading of two anticancer drugs on the GO surface was achieved by Zhang and coworkers, who used GO functionalized with folic acid to convey two water-insoluble cancer drugs, camptothecin and doxorubicin, to specifically treat MCF-7 human breast cancer cells.49 Recent reports also demonstrate that GO can act as a photothermal agent for medical treatment.50–53
Aptamers, a new class of targeting ligands, have been selected and amplified for specific targets. A wide range of targets, including metal ions (Pb2+, Cd2+), small molecules (cocaine, adenosine triphosphate), proteins (protein tyrosine kinase 7, immunoglobulin G, nucleolin and thrombin) and even whole viruses (human influenza B), bacteria (methicillin-resistant Staphylococcus aureus (MRSA)) and cancer (T-cell acute lymphoblastic leukemia, B lymphocyte and MCF-7 human breast cancer) cells, has been used to generate single-stranded DNA- or RNA-based aptamers by a process termed “SELEX” (systematic evolution of ligands by exponential enrichment) with dissociation constants (Kd) in the micromolar to nanomolar (nM), or even picomolar (pM), ranges.54–62 Aptamers have received considerable attention by bioscience researchers because of their exceptional properties, including flexibility, reproducibility in the selection and synthesis protocol, low molecular weight, low immune response, reversible denaturation, easy chemical modification, and stability.63 Tan and coworkers have isolated and identified aptamers using whole living cells via a new technique known as cell-SELEX, which produces aptamers that bind with high affinity and selectivity to receptors, typically a protein, on the membranes of target cells. Thus, early diagnosis and targeted therapy have been successfully accomplished by using aptamer recognition of molecular signatures on target cells.53,57
In this work, we developed a multifunctional hybrid nanostructure capable of providing targeted PTT and PDT. First, we synthesized magnetic graphene oxide (mGO) to utilize as a platform for loading ICG dye via π–π stacking. Then, the edges of mGO were functionalized with sgc8 DNA aptamers as targeting ligands for binding to target cells. Magnetic-GO and ICG have been separately considered as photothermal agents. With NIR light irradiation, Apt@ICG@mGO exhibits a cooperative effect by generating high local heat reaching 43 °C in 20 seconds. However, ICG, as a PDT agent, also produces singlet oxygen under NIR laser irradiation. Thus, the combination of PTT and PDT enhances target cancer cell killing efficiency. Our results show the Apt@ICG@mGO conjugate to be a promising nanostructure system for effective light-induced cancer cell destruction by enhanced PTT and PDT.
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| Fig. 1 Schematic illustration of synthesis of mGO, Apt@ICG@mGO and cancer cell death through PTT and PDT. | ||
GO, mGO and ICG@mGO were characterized via transmission electron microscopy (TEM), Fourier transform infrared spectroscopy (FTIR) and UV-vis spectrometry. Fig. 2A shows the TEM image of bare GO in pieces of various sizes. Fe3O4 NPs grown on GO (1
:
1 weight ratio) were clearly observed by TEM (Fig. 2B). The different weight ratios of Fe(acac)3/GO nano powder (5
:
1, 4
:
1 and 2
:
1) changed the number of Fe3O4 NPs on the surface of GO (Fig. S1 in the ESI data†). The color of GO in aqueous solution was brown (Fig. 2C(i)), while the color of mGO became black after formation of Fe3O4 NPs on the surface of GO (Fig. 2C(ii)). The photograph in Fig. 2C(ii) also shows that mGO is highly water-soluble and stable in aqueous solution without any aggregation. The mGO dispersed in PBS solution was accumulated on the wall of a glass vial, demonstrating the magnetic property of mGO (Fig. 2C(iii)). It should be noted that accumulated mGO remained on the vial wall for a long time, even after the external magnetic field (magnet) was removed (Fig. 2C(iv)).
Free ICG with various concentrations dissolved in ethanol or water exhibited a characteristic absorption peak around 780 nm (Fig. 2D). Free ICG in aqueous solution forms aggregates in a short time, depending on its concentration, and it is also rapidly degraded. ICG at low concentrations (≤129 μM) exhibits single or double sharp absorption peak(s), while concentrations of ICG greater than 129 μM show a very broad peak between 780 and 590 nm, which is also an indication of agglomeration of ICG monomers (Fig. S2 in the ESI data†). After loading ICG on the mGO surface via pi-electron delocalization, a characteristic peak of ICG appeared around 808 nm (28 nm red shift), which matched the wavelength of the NIR laser used for PTT and PDT (Fig. 2D). In addition, mGO was used as both carrier and stabilizer to prevent aggregation of ICG. FTIR spectra were obtained for ICG and ICG@mGO (Fig. 2E). For mGO, the O–H stretching vibration appeared at 3437 cm−1, and aromatic C
C and carboxyl stretching vibrations appeared at 1599 cm−1 and 1384 cm−1, respectively. The vibration of C–O in the epoxy group appeared at 1114 cm−1. For ICG@mGO, the vibrational stretching of C
N and C
C appeared at 1602 cm−1 and 1414 cm−1, respectively, while the vibrational stretching of single-bond C–N appeared at 1352 cm−1. All of these stretching vibrations were present in ICG. The stretching vibrations of S
O (1089 cm−1), C–S and S–O (1089 cm−1) were also indications of successful conjugation of ICG on the surface of mGO. Carbon–oxygen vibration (C–O–C) at 854 and 1088 cm−1 appeared.
Singlet oxygen generation (1O2) is a key component for PDT. The extent of 1O2 produced by free ICG and ICG@mGO was determined on the basis of decreased absorbance of N,N-dimethyl-4-nitrosoaniline (RNO) via UV-vis spectroscopy. The mixture of free ICG and RNO was irradiated with the 808 nm NIR laser, and the absorbance of RNO at 440 nm decreased as a result of 1O2 production (Fig. 3A). When the mixture of mGO and RNO was exposed to NIR laser irradiation, the generation of 1O2 was not observed (Fig. 3B). Although mGO almost completely quenched the fluorescence of ICG loaded on its surface in the ICG@mGO conjugate, it is interesting that ICG was still partially capable of producing 1O2 under NIR laser irradiation (Fig. 3C). This can be explained by the structural differences of GO compared to other carbon-based materials. For instance, GO may have surface defects, which cause slight energy absorption. We proved that RNO itself did not generate any 1O2, even though it was exposed to NIR laser irradiation for 10 min (Fig. S3 in the ESI data†). Note that ICG and ICG@mGO without light irradiation were unable to generate 1O2, as shown by the red line in Fig. 3A and C. Furthermore, the fluorescence spectra of ICG and ICG@mGO showed fluorescence interaction between ICG and mGO. More than 95% of ICG fluorescence was quenched after it was loaded on the surface of mGO (Fig. 3D).
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| Fig. 3 Singlet generation of (A) ICG, (B) GO and (C) ICG@mGO. (D) Fluorescence intensities of ICG and ICG@mGO at different concentrations. | ||
To show the heat generation capability of mGO, free ICG and ICG@mGO, each material was dissolved in PBS solution and irradiated with the 808 nm laser for 5 min (Fig. 4). The mGO (50 μg mL−1) caused an increase in temperature from ∼24 °C to ∼58 °C within 5 min, while free ICG solution (5 μM) reached ∼54 °C. However, the ICG@(5 μM)mGO (50 μg mL−1) conjugate dramatically increased the temperature from ∼24 °C to ∼76 °C. Within 40 s, we observed that the ICG@mGO conjugate reached ∼51 °C, which can destroy all types of cancer cells. We conclude that the ICG@mGO conjugate causes a temperature increase greater than that of either mGO or free ICG alone. We speculate that the 28 nm shift in the λmax of ICG to 808 nm, as shown Fig. 2D, provided rapid and abundant heat production.
Binding of Apt@ICG@mGO to the target CCRF-CEM cells was performed at 37 °C for 2 h (Fig. 5A). First, one million CCRF-CEM cells were prepared in seven separate tubes. Tube 1 contained only cells without any aptamer or hetero-nanostructures, while tubes 2 and 3 were mixed with free library DNA and sgc8 aptamer, respectively. Tube 4 contained only ICG@mGO without aptamer, while tubes 5, 6, and 7 included Apt@ICG@mGO conjugates with respective concentrations of 10, 100 and 200 ng mL−1. All tubes were incubated in an incubator shaker at 250 rpm (Forma Refrigerated Orbital Shaker, Thermo Electron Corp., Asheville, NC, USA) at 37 °C for 2 h. After incubation, the contents of each tube were washed with washing buffer and redispersed in binding buffer prior to flow cytometry. The fluorescence signal, as an indication of cell binding and internalization, was not observed with cells only (red line). The FTIC-labeled library DNA used as a control did not show any binding to target cells, as expected (light green line). However, a significant right shift was observed with the mixture of cells and FITC-labeled sgc8 aptamer because this aptamer specifically bound and entered the target cells (blue line). No binding or internalization was observed with ICG@mGO conjugates without aptamer. In contrast, sgc8 aptamer-functionalized ICG@mGO conjugates resulted in successful binding and internalization. Furthermore, the fluorescence signal intensities, as right shifts, increased with increasing concentrations of sgc8 Apt@ICG@mGO conjugates from 10 ng mL−1 (brown line) to 100 ng mL−1 (dark green) and 200 ng mL−1 (orange line).
To assess the efficiency of PTT and PDT, cell viability tests were performed with only cells (a), mGO (b), free ICG (c), ICG@mGO (d), sgc8@mGO (e), sgc8@ICG@mGO (f) and rDNA@ICG@mGO (g) (10, 50, 100 ppm) under nonilluminated and illuminated conditions. It is worthy to mention that the light activates both PTT and PDT agents (GO and ICG) which kills the cancer cells. Without light, these biocompatible agents are harmless. Target CCRF-CEM cells were separately incubated with each structure aforementioned, followed by non-irradiation and 808 nm laser irradiation at 1.1 W cm−2 for 5 min, respectively. The mGO, utilized as photothermal agent, generated heat for PTT. However, the ICG@mGO conjugate served as both a photothermal and a photodynamic agent owing to the presence of ICG. Thus, the enhanced PTT, based on the heat generated both from ICG and mGO, and PDT, based on the production of 1O2 by ICG, led to effective destruction of target cancer cells. However, the regardless of structures and their dosages, there was no reduction in the number of live cancer cells under the nonilluminated condition (without 808 nm laser irradiation) as shown in Fig. 5B. In contrast to that, when 808 nm NIR laser irradiation was exposed to structures for 5 min, the cancer cell destruction was observed (Fig. 5C). Although only cell solution was illuminated with NIR laser, no cell destruction was seen due to absence of structures generating heat or 1O2.
For instance, when NIR laser irradiation was introduced, mGO conjugates only killed ∼9% and ∼13% and ∼20% of cell with respective concentrations (10, 50 and 100 ppm) while free ICG induced ∼6% and ∼11% and ∼17%. However, a slight increase in cell killing stated 7% and ∼19% and ∼24% when ICG@mGO conjugates used at the same respective concentrations above. None of these conjugates was not functionalized with aptamer, due to that they were lack of binding target cell. After incubation of the mixture of target cell and these conjugates, the most of conjugates were removed from the mixture by centrifugation except a little amount of nonspecifically binding one. The aptamer functionalized sgc8@mGO decreased the survival rate of CCRF-CEM cells by killing ∼32%, ∼40% and ∼50% of CCRF-CEM cells at 10, 50 and 100 ppm, respectively while sgc8@ICG@mGO showed dramatic reduction in cell viability with 41%, ∼60% and ∼82% (Fig. 5C). To prove the function of aptamer for enhancing the cell-killing ability of conjugates, we also immobilized ICG@mGO with random DNA (rDNA@ICG@mGO). We demonstrated that rDNA@ICG@mGO only killed ∼21% of CCRF-CEM cells at 100 ppm. This result also support function and importance of aptamer for targeting target cell. We conclude that the rapid increase in heat generated from both ICG and mGO and generation of 1O2 from ICG components of ICG@mGO conjugates combined with targeting capability of sgc8 aptamer the resulted in enhanced dual PT and PD therapies for effectively and rapidly killing of CCRF-CEM cells.
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1) at 65 °C for 30 min. After deprotection, all sequences were purified by reversed-phase HPLC (ProStar-Varian, Walnut Creek, CA) with a C18 column (Econosil, 5 μm, 250 mm length, 4.6 mm diameter) from Alltech (Deerfield, IL) using a mobile phase containing 100 mM triethylamine acetic acid buffer (TEAA, pH 7.5) and acetonitrile (0–30 min, 10–00%). All purified DNA solutions were dried in acid-resistant centriVap centrifugal vacuum concentrators (Labconco, Kansas City, MO). The dried DNA at the bottom of 2 mL tubes was dissolved in 50–100 μL of DNA grade water. The concentrations of all DNA were determined by measuring the absorbance values at 260 nm.
Detection of singlet oxygen generation: to determine the generation of singlet oxygen, known concentrations of mGO, ICG and ICG@mGO were mixed with N,N-dimethyl-4-nitrosoaniline (RNO) (20 μM) and imidazole (20 μM) in 1 mL 10 mM PBS solution (pH 7.4). Each resulting mixture was illuminated at 808 nm using a near-infrared (NIR) laser with power of 1.1 W cm−2 for different periods of time. The reduction of RNO absorption at 440 nm indicated the generation of singlet oxygen from each sample (mGO, ICG and ICG@mGO).
Footnote |
| † Electronic supplementary information (ESI) available: TEM images of mGO, ICG concentration-dependent absorption spectra and RNO absorption spectra recorded after time increments of NIR laser irradiation. See DOI: 10.1039/c6ra06798k |
| This journal is © The Royal Society of Chemistry 2016 |